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Please see the license in the file LICENSE and URL above * 16 // * for the full disclaimer and the limitatio 16 // * for the full disclaimer and the limitation of liability. * 17 // * 17 // * * 18 // * This code implementation is the result 18 // * This code implementation is the result of the scientific and * 19 // * technical work of the GEANT4 collaboratio 19 // * technical work of the GEANT4 collaboration. * 20 // * By using, copying, modifying or distri 20 // * By using, copying, modifying or distributing the software (or * 21 // * any work based on the software) you ag 21 // * any work based on the software) you agree to acknowledge its * 22 // * use in resulting scientific publicati 22 // * use in resulting scientific publications, and indicate your * 23 // * acceptance of all terms of the Geant4 Sof 23 // * acceptance of all terms of the Geant4 Software license. * 24 // ******************************************* 24 // ******************************************************************** 25 // 25 // >> 26 // $Id: G4KleinNishinaCompton.cc 74309 2013-10-03 06:42:30Z gcosmo $ 26 // 27 // 27 // ------------------------------------------- 28 // ------------------------------------------------------------------- 28 // 29 // 29 // GEANT4 Class file 30 // GEANT4 Class file 30 // 31 // 31 // 32 // 32 // File name: G4KleinNishinaCompton 33 // File name: G4KleinNishinaCompton 33 // 34 // 34 // Author: Vladimir Ivanchenko on base 35 // Author: Vladimir Ivanchenko on base of Michel Maire code 35 // 36 // 36 // Creation date: 15.03.2005 37 // Creation date: 15.03.2005 37 // 38 // 38 // Modifications: 39 // Modifications: 39 // 18-04-05 Use G4ParticleChangeForGamma (V.Iv 40 // 18-04-05 Use G4ParticleChangeForGamma (V.Ivantchenko) 40 // 27-03-06 Remove upper limit of cross sectio 41 // 27-03-06 Remove upper limit of cross section (V.Ivantchenko) 41 // 42 // 42 // Class Description: 43 // Class Description: 43 // 44 // 44 // ------------------------------------------- 45 // ------------------------------------------------------------------- 45 // 46 // 46 //....oooOO0OOooo........oooOO0OOooo........oo 47 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 47 //....oooOO0OOooo........oooOO0OOooo........oo 48 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 48 49 49 #include "G4KleinNishinaCompton.hh" 50 #include "G4KleinNishinaCompton.hh" 50 #include "G4PhysicalConstants.hh" 51 #include "G4PhysicalConstants.hh" 51 #include "G4SystemOfUnits.hh" 52 #include "G4SystemOfUnits.hh" 52 #include "G4Electron.hh" 53 #include "G4Electron.hh" 53 #include "G4Gamma.hh" 54 #include "G4Gamma.hh" 54 #include "Randomize.hh" 55 #include "Randomize.hh" 55 #include "G4DataVector.hh" 56 #include "G4DataVector.hh" 56 #include "G4ParticleChangeForGamma.hh" 57 #include "G4ParticleChangeForGamma.hh" 57 #include "G4Log.hh" 58 #include "G4Log.hh" 58 #include "G4Exp.hh" 59 #include "G4Exp.hh" 59 60 60 //....oooOO0OOooo........oooOO0OOooo........oo 61 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 61 62 62 using namespace std; 63 using namespace std; 63 64 >> 65 static const G4double >> 66 d1= 2.7965e-1*barn, d2=-1.8300e-1*barn, d3= 6.7527 *barn, d4=-1.9798e+1*barn, >> 67 e1= 1.9756e-5*barn, e2=-1.0205e-2*barn, e3=-7.3913e-2*barn, e4= 2.7079e-2*barn, >> 68 f1=-3.9178e-7*barn, f2= 6.8241e-5*barn, f3= 6.0480e-5*barn, f4= 3.0274e-4*barn; >> 69 64 G4KleinNishinaCompton::G4KleinNishinaCompton(c 70 G4KleinNishinaCompton::G4KleinNishinaCompton(const G4ParticleDefinition*, 65 c 71 const G4String& nam) 66 : G4VEmModel(nam) 72 : G4VEmModel(nam) 67 { 73 { 68 theGamma = G4Gamma::Gamma(); 74 theGamma = G4Gamma::Gamma(); 69 theElectron = G4Electron::Electron(); 75 theElectron = G4Electron::Electron(); 70 lowestSecondaryEnergy = 100.0*eV; << 76 lowestGammaEnergy = 1.0*eV; 71 fParticleChange = nullptr; << 77 fParticleChange = 0; 72 } 78 } 73 79 74 //....oooOO0OOooo........oooOO0OOooo........oo 80 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 75 81 76 G4KleinNishinaCompton::~G4KleinNishinaCompton( << 82 G4KleinNishinaCompton::~G4KleinNishinaCompton() >> 83 {} 77 84 78 //....oooOO0OOooo........oooOO0OOooo........oo 85 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 79 86 80 void G4KleinNishinaCompton::Initialise(const G 87 void G4KleinNishinaCompton::Initialise(const G4ParticleDefinition* p, 81 const G 88 const G4DataVector& cuts) 82 { 89 { 83 if(IsMaster()) { InitialiseElementSelectors( 90 if(IsMaster()) { InitialiseElementSelectors(p, cuts); } 84 if(nullptr == fParticleChange) { << 91 if(!fParticleChange) { fParticleChange = GetParticleChangeForGamma(); } 85 fParticleChange = GetParticleChangeForGamm << 86 } << 87 } 92 } 88 93 89 //....oooOO0OOooo........oooOO0OOooo........oo 94 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 90 95 91 void G4KleinNishinaCompton::InitialiseLocal(co 96 void G4KleinNishinaCompton::InitialiseLocal(const G4ParticleDefinition*, 92 G4 << 97 G4VEmModel* masterModel) 93 { 98 { 94 SetElementSelectors(masterModel->GetElementS 99 SetElementSelectors(masterModel->GetElementSelectors()); 95 } 100 } 96 101 97 //....oooOO0OOooo........oooOO0OOooo........oo 102 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 98 103 99 G4double G4KleinNishinaCompton::ComputeCrossSe 104 G4double G4KleinNishinaCompton::ComputeCrossSectionPerAtom( 100 const G 105 const G4ParticleDefinition*, 101 G 106 G4double GammaEnergy, 102 G 107 G4double Z, G4double, 103 G 108 G4double, G4double) 104 { 109 { 105 G4double xSection = 0.0 ; 110 G4double xSection = 0.0 ; 106 if (GammaEnergy <= LowEnergyLimit()) { retur << 111 if ( Z < 0.9999 ) return xSection; >> 112 if ( GammaEnergy < 0.1*keV ) return xSection; >> 113 // if ( GammaEnergy > (100.*GeV/Z) ) return xSection; 107 114 108 static const G4double a = 20.0 , b = 230.0 , 115 static const G4double a = 20.0 , b = 230.0 , c = 440.0; 109 << 110 static const G4double << 111 d1= 2.7965e-1*CLHEP::barn, d2=-1.8300e-1*CLH << 112 d3= 6.7527 *CLHEP::barn, d4=-1.9798e+1*CLH << 113 e1= 1.9756e-5*CLHEP::barn, e2=-1.0205e-2*CLH << 114 e3=-7.3913e-2*CLHEP::barn, e4= 2.7079e-2*CLH << 115 f1=-3.9178e-7*CLHEP::barn, f2= 6.8241e-5*CLH << 116 f3= 6.0480e-5*CLHEP::barn, f4= 3.0274e-4*CLH << 117 116 118 G4double p1Z = Z*(d1 + e1*Z + f1*Z*Z), p2Z = 117 G4double p1Z = Z*(d1 + e1*Z + f1*Z*Z), p2Z = Z*(d2 + e2*Z + f2*Z*Z), 119 p3Z = Z*(d3 + e3*Z + f3*Z*Z), p4Z = 118 p3Z = Z*(d3 + e3*Z + f3*Z*Z), p4Z = Z*(d4 + e4*Z + f4*Z*Z); 120 119 121 G4double T0 = 15.0*keV; 120 G4double T0 = 15.0*keV; 122 if (Z < 1.5) { T0 = 40.0*keV; } << 121 if (Z < 1.5) T0 = 40.0*keV; 123 122 124 G4double X = max(GammaEnergy, T0) / electr 123 G4double X = max(GammaEnergy, T0) / electron_mass_c2; 125 xSection = p1Z*G4Log(1.+2.*X)/X 124 xSection = p1Z*G4Log(1.+2.*X)/X 126 + (p2Z + p3Z*X + p4Z*X*X)/(1. + 125 + (p2Z + p3Z*X + p4Z*X*X)/(1. + a*X + b*X*X + c*X*X*X); 127 << 126 128 // modification for low energy. (special ca 127 // modification for low energy. (special case for Hydrogen) 129 if (GammaEnergy < T0) { 128 if (GammaEnergy < T0) { 130 static const G4double dT0 = keV; << 129 G4double dT0 = 1.*keV; 131 X = (T0+dT0) / electron_mass_c2 ; 130 X = (T0+dT0) / electron_mass_c2 ; 132 G4double sigma = p1Z*G4Log(1.+2*X)/X 131 G4double sigma = p1Z*G4Log(1.+2*X)/X 133 + (p2Z + p3Z*X + p4Z*X*X)/ 132 + (p2Z + p3Z*X + p4Z*X*X)/(1. + a*X + b*X*X + c*X*X*X); 134 G4double c1 = -T0*(sigma-xSection)/(xSec 133 G4double c1 = -T0*(sigma-xSection)/(xSection*dT0); 135 G4double c2 = 0.150; 134 G4double c2 = 0.150; 136 if (Z > 1.5) { c2 = 0.375-0.0556*G4Log(Z); << 135 if (Z > 1.5) c2 = 0.375-0.0556*G4Log(Z); 137 G4double y = G4Log(GammaEnergy/T0); 136 G4double y = G4Log(GammaEnergy/T0); 138 xSection *= G4Exp(-y*(c1+c2*y)); 137 xSection *= G4Exp(-y*(c1+c2*y)); 139 } 138 } 140 // G4cout<<"e= "<< GammaEnergy<<" Z= "<<Z<<" << 139 // G4cout << "e= " << GammaEnergy << " Z= " << Z << " cross= " << xSection << G4endl; 141 return xSection; 140 return xSection; 142 } 141 } 143 142 144 //....oooOO0OOooo........oooOO0OOooo........oo 143 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... 145 144 146 void G4KleinNishinaCompton::SampleSecondaries( << 145 void G4KleinNishinaCompton::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect, 147 std::vector<G4Dyna << 146 const G4MaterialCutsCouple*, 148 const G4MaterialCu << 147 const G4DynamicParticle* aDynamicGamma, 149 const G4DynamicPar << 148 G4double, 150 G4double, << 149 G4double) 151 G4double) << 152 { 150 { 153 // The scattered gamma energy is sampled acc 151 // The scattered gamma energy is sampled according to Klein - Nishina formula. 154 // The random number techniques of Butcher & 152 // The random number techniques of Butcher & Messel are used 155 // (Nuc Phys 20(1960),15). 153 // (Nuc Phys 20(1960),15). 156 // Note : Effects due to binding of atomic e 154 // Note : Effects due to binding of atomic electrons are negliged. 157 155 158 G4double gamEnergy0 = aDynamicGamma->GetKine 156 G4double gamEnergy0 = aDynamicGamma->GetKineticEnergy(); 159 157 160 // do nothing below the threshold << 158 // extra protection 161 if(gamEnergy0 <= LowEnergyLimit()) { return; << 159 if(gamEnergy0 < lowestGammaEnergy) { >> 160 fParticleChange->ProposeTrackStatus(fStopAndKill); >> 161 fParticleChange->ProposeLocalEnergyDeposit(gamEnergy0); >> 162 fParticleChange->SetProposedKineticEnergy(0.0); >> 163 return; >> 164 } 162 165 163 G4double E0_m = gamEnergy0 / electron_mass_c 166 G4double E0_m = gamEnergy0 / electron_mass_c2 ; 164 167 165 G4ThreeVector gamDirection0 = aDynamicGamma- 168 G4ThreeVector gamDirection0 = aDynamicGamma->GetMomentumDirection(); 166 169 167 // 170 // 168 // sample the energy rate of the scattered g 171 // sample the energy rate of the scattered gamma 169 // 172 // 170 173 171 G4double epsilon, epsilonsq, onecost, sint2, 174 G4double epsilon, epsilonsq, onecost, sint2, greject ; 172 175 173 G4double eps0 = 1./(1. + 2.*E0_m); 176 G4double eps0 = 1./(1. + 2.*E0_m); 174 G4double epsilon0sq = eps0*eps0; 177 G4double epsilon0sq = eps0*eps0; 175 G4double alpha1 = - G4Log(eps0); 178 G4double alpha1 = - G4Log(eps0); 176 G4double alpha2 = alpha1 + 0.5*(1.- epsi << 179 G4double alpha2 = 0.5*(1.- epsilon0sq); 177 << 178 CLHEP::HepRandomEngine* rndmEngineMod = G4Ra << 179 G4double rndm[3]; << 180 180 181 static const G4int nlooplim = 1000; << 182 G4int nloop = 0; << 183 do { 181 do { 184 ++nloop; << 182 if ( alpha1/(alpha1+alpha2) > G4UniformRand() ) { 185 // false interaction if too many iteration << 183 epsilon = G4Exp(-alpha1*G4UniformRand()); // eps0**r 186 if(nloop > nlooplim) { return; } << 187 << 188 // 3 random numbers to sample scattering << 189 rndmEngineMod->flatArray(3, rndm); << 190 << 191 if ( alpha1 > alpha2*rndm[0] ) { << 192 epsilon = G4Exp(-alpha1*rndm[1]); // << 193 epsilonsq = epsilon*epsilon; 184 epsilonsq = epsilon*epsilon; 194 185 195 } else { 186 } else { 196 epsilonsq = epsilon0sq + (1.- epsilon0sq << 187 epsilonsq = epsilon0sq + (1.- epsilon0sq)*G4UniformRand(); 197 epsilon = sqrt(epsilonsq); 188 epsilon = sqrt(epsilonsq); 198 }; 189 }; 199 190 200 onecost = (1.- epsilon)/(epsilon*E0_m); 191 onecost = (1.- epsilon)/(epsilon*E0_m); 201 sint2 = onecost*(2.-onecost); 192 sint2 = onecost*(2.-onecost); 202 greject = 1. - epsilon*sint2/(1.+ epsilons 193 greject = 1. - epsilon*sint2/(1.+ epsilonsq); 203 194 204 // Loop checking, 03-Aug-2015, Vladimir Iv << 195 } while (greject < G4UniformRand()); 205 } while (greject < rndm[2]); << 206 196 207 // 197 // 208 // scattered gamma angles. ( Z - axis along 198 // scattered gamma angles. ( Z - axis along the parent gamma) 209 // 199 // 210 200 211 if(sint2 < 0.0) { sint2 = 0.0; } 201 if(sint2 < 0.0) { sint2 = 0.0; } 212 G4double cosTeta = 1. - onecost; 202 G4double cosTeta = 1. - onecost; 213 G4double sinTeta = sqrt (sint2); 203 G4double sinTeta = sqrt (sint2); 214 G4double Phi = twopi * rndmEngineMod->fl << 204 G4double Phi = twopi * G4UniformRand(); 215 205 216 // 206 // 217 // update G4VParticleChange for the scattere 207 // update G4VParticleChange for the scattered gamma 218 // 208 // 219 209 220 G4ThreeVector gamDirection1(sinTeta*cos(Phi) 210 G4ThreeVector gamDirection1(sinTeta*cos(Phi), sinTeta*sin(Phi), cosTeta); 221 gamDirection1.rotateUz(gamDirection0); 211 gamDirection1.rotateUz(gamDirection0); 222 G4double gamEnergy1 = epsilon*gamEnergy0; 212 G4double gamEnergy1 = epsilon*gamEnergy0; 223 G4double edep = 0.0; << 213 if(gamEnergy1 > lowestGammaEnergy) { 224 if(gamEnergy1 > lowestSecondaryEnergy) { << 225 fParticleChange->ProposeMomentumDirection( 214 fParticleChange->ProposeMomentumDirection(gamDirection1); 226 fParticleChange->SetProposedKineticEnergy( 215 fParticleChange->SetProposedKineticEnergy(gamEnergy1); 227 } else { 216 } else { 228 fParticleChange->ProposeTrackStatus(fStopA 217 fParticleChange->ProposeTrackStatus(fStopAndKill); >> 218 fParticleChange->ProposeLocalEnergyDeposit(gamEnergy1); 229 fParticleChange->SetProposedKineticEnergy( 219 fParticleChange->SetProposedKineticEnergy(0.0); 230 edep = gamEnergy1; << 231 } 220 } 232 221 233 // 222 // 234 // kinematic of the scattered electron 223 // kinematic of the scattered electron 235 // 224 // 236 225 237 G4double eKinEnergy = gamEnergy0 - gamEnergy 226 G4double eKinEnergy = gamEnergy0 - gamEnergy1; 238 227 239 if(eKinEnergy > lowestSecondaryEnergy) { << 228 if(eKinEnergy > DBL_MIN) { 240 G4ThreeVector eDirection = gamEnergy0*gamD 229 G4ThreeVector eDirection = gamEnergy0*gamDirection0 - gamEnergy1*gamDirection1; 241 eDirection = eDirection.unit(); 230 eDirection = eDirection.unit(); 242 231 243 // create G4DynamicParticle object for the 232 // create G4DynamicParticle object for the electron. 244 auto dp = new G4DynamicParticle(theElectro << 233 G4DynamicParticle* dp = new G4DynamicParticle(theElectron,eDirection,eKinEnergy); 245 fvect->push_back(dp); 234 fvect->push_back(dp); 246 } else { << 247 edep += eKinEnergy; << 248 } << 249 // energy balance << 250 if(edep > 0.0) { << 251 fParticleChange->ProposeLocalEnergyDeposit << 252 } 235 } 253 } 236 } 254 237 255 //....oooOO0OOooo........oooOO0OOooo........oo 238 //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo...... 256 239 257 240 258 241